4.8 Article

Structure inversion asymmetry enhanced electronic structure and electrical transport in 2D A3SnO (A = Ca, Sr, and Ba) anti-perovskite monolayers

期刊

NANO RESEARCH
卷 16, 期 1, 页码 1779-1791

出版社

TSINGHUA UNIV PRESS
DOI: 10.1007/s12274-022-4637-3

关键词

electrical transport; anti-perovskites; low-dimensional materials; electronic structure; mechanical properties

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Anti-perovskite A(3)SnO (A = Ca, Sr, and Ba) monolayers exhibit interesting electronic properties, including Rashba-type splitting and Dirac cone, due to crystal symmetry, spin-orbit coupling, and band overlap. The monolayers Ca3SnO and Sr3SnO show superior thermoelectric performance compared to their bulk counterparts due to inversion asymmetry.
Anti-perovskites A(3)SnO (A = Ca, Sr, and Ba) are an important class of materials due to the emergence of Dirac cones and tiny mass gaps in their band structures originating from an intricate interplay of crystal symmetry, spin-orbit coupling, and band overlap. This provides an exciting playground for modulating their electronic properties in the two-dimensional (2D) limit. Herein, we employ first-principles density functional theory (DFT) calculations by combining dispersion-corrected SCAN + rVV10 and mBJ functionals for a comprehensive side-by-side comparison of the structural, thermodynamic, dynamical, mechanical, electronic, and thermoelectric properties of bulk and monolayer (one unit cell thick) A(3)SnO anti-perovskites. Our results show that 2D monolayers derived from bulk A(3)SnO anti-perovskites are structurally and energetically stable. Moreover, Rashba-type splitting in the electronic structure of Ca3SnO and Sr3SnO monolayers is observed owing to strong spin-orbit coupling and inversion asymmetry. On the other hand, monolayer Ba3SnO exhibits Dirac cone at the high-symmetry Gamma point due to the domination of band overlap. Based on the predicted electronic transport properties, it is shown that inversion asymmetry plays an essential character such that the monolayers Ca3SnO and Sr3SnO outperform thermoelectric performance of their bulk counterparts.

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